GB2164747A

GB2164747A - Magnetic field sensors

Info

Publication number: GB2164747A
Application number: GB08523434A
Authority: GB
Inventors: Stafford Malcolm Ellis; Donald Roy Charles Price
Original assignee: GEC Avionics Ltd
Current assignee: Allard Way Holdings Ltd
Priority date: 1984-09-24
Filing date: 1985-09-23
Publication date: 1986-03-26
Also published as: FR2570833A1; FR2570833B3; GB8523434D0; US4656421A

Description

1 GB2164747A 1

SPECIFICATION

Magnetic field sensors

This invention relates to magnetic field sen- 70 sors.

In recent years a number of so called optical fibre magnetic field sensors have been devel oped. Examples of three such sensors are shown in the review article -Optical Fiber Sen sor Technology-, published on pages 626-665 of the IEEE Journal of Quantum Elhctronics, Vol. QE-18 No. 4, April 1982.

Each sensor comprises a magnetostrictive ele ment, a single mode optical fibre being bonded along its length to the element. Any change in magnetic field will produce a varia tion in the size of the magnetostrictive ele ment, which as a result of its bonding to the optical fibre will produce a strain in the fibre.

This strain gives rise to an optical phase change, which may be measured, for example in an interferometer of which the fibre forms a part. In the first particular sensor described in the article, the magnetostrictive element is in the form of a mandrel, round which the fibre is wound, in the second sensor the element is a coating on the fibre, whilst in the third sen sor the element is an elongate strip along which the fibre runs.

In the coating and elongate strip arrange ments, the sensitivity of the sensor is deter mined by the length of the coating or strip to which the fibre is attached, this producing a limit on the minimum length of the device.

Whilst in the mandrel arrangement, this problem is overcome, the form of the magne tostrictive element means that it has no direc tional sensitivity within its plane of sensitivity.

Furthermore in each of these arrangements it is necessary to attach the fibre along its length to the magnetostrictive element.

It is an object of the present invention to provide an alternative form of optical fibre magnetic field sensor wherein these difficulties may be alleviated.

According to the present invention a magnetic field sensor comprises an arcuate element comprising two superimposed elongate strips of material, the magnetostrictive constant along the longitudinal axis of one of the strips being greater than that of the other strip; and means for attaching an optical fibre along a chord of the element such that a vari- ation in applied magnetic field in the plane containing the arc of the element gives rise to a variation in the curvature of the element so as to produce a variation in the strain in the fibre.

optical phase of light passing through the fibre.

The material of said one strip is suitably a metallic glass.

One particular magnetic field sensor in ac cordance with the invention, together with an interferometer incorporating the sensor, will now be described, by way of example only, with reference to the accompanying drawings in which:

Figure 1 is a schematic side view of the sensor; Figure 2 is a section along the line 11-11 of Fig. 1; and Figure 3 is a schematic diagram of an inter ferometer incorporating the sensor.

Referring firstly to Figs. 1 and 2 the sensor comprises an arcuate metallic element, com prising a strip of metal of low magnetostric tive constant 1 to which is bonded a strip of a metallic glass 3, for example FeBSi. The ends of the strip 1 extend beyond the strip 3, a respective post 5a or 5b being provided at each end. A single mode optical fibre 7 is secured to the bimetallic element, by being wound round and glued to each post, such that the portion of the fibre between the posts 5a, 5b is taut so as to form a chord of the arc defined by the bimetallic element.

Referring now also to Fig. 3, the sensor is incorporated in a Mach-Zehnder interferometer.

This comprises a single mode laser 9 which produces a beam which is split by a beam splitter arrangement 11 between the fibre 7 and a reference fibre 13. Part of the reference fibre 13 is wound round and glued to a piezo electric cylinder 15. The beams passing through the fibres 7, 13 are combined in a combiner 17 to produce two complementary beams which are detected by respective de tectors 19, 21 whose outputs are connected to a phase tracking electronics arrangement 23 which is in turn connected to an arrange ment 25 for providing a voltage across the piezoelectric cylinder 15.

In use of the interferometer to monitor changes in a DC magnetic field applied in the plane containing the arc defined by the bime tallic element, an AC bias magnetic field is applied in this plane. The resultant varying magnetic field will cause changes in the length of the strip 3 relative to that of the strip 1.

This will cause changes in curvature of the element, consequential changes in the strain in the part of the fibre 7 between the posts 5a, 5b being produced. The phase of the light passing through the fibre 7 will therefore change relative to the phase of the light pass ing through the fibre 13, this phase change being detected by the detectors 19, 21. By using the phase tracking electronics arrange ment 23 and arrangement 25 to apply a feed back voltage to the piezoelectric cylinder 15, The fibre is suitably part of a Mach-Zehnder the phase change produced by the strain pro- interferometer arranged to monitor changes in 130duced in the reference fibre 13 by its attach- The means for attaching suitably comprises 125 a pair of posts, one at each end of the chord.

These posts preferably project from said other strip.

2 GB2164747A 2 ment to the piezoelectric cylinder may be used to cause to two outputs of the detectors 19, 21 to be maintained at their quadrature points i.e. to phase lock the system. This -active homodyne- detection system enables amplitude fluctuations in the light from the laser common to both arms of the interferometer to cancel out.

Any subsequent changes in the DC field be- ing monitored produce a corresponding change in the output signal produced by the interferometer which is thus indicative of the strength of the DC magnetic field.

For a semi-circular arc, the sensitivity to the field of the sensor is approximately uniform in the plane of the arc, failing off cosinusoidally out of the plane. If however the bimetallic element is bow shaped, a directional sensitivity within the plane of the arc is achieved.

The design of the actual sensor, apart from considerations of mechanical strength, generally focusses on two principal criteria. One is the 'mechanical' gain K defined as the relative unloaded extension of the chord defined by the part of the optical fibre 7 between the posts divided by difference between the relative extensions of the components of the bimetallic element.

Bimetallic strip theory as for example given in -Engineering- published September, 1961 pages 1 to 12 indicates that in the case of a semi-circular bimetallic strip this ratio K is approximately given by 3R K=- 2t where R is the radius of the semi-circle and t is the thickness of the strips where R is 25mm, and t is lmm, a value of K of 37.5 is achieved. Thus a more sensitive device may be obtained than with known optical fibre magnetic field sensors.

The second design criterion is a preference to drive the sensor at a high frequency typically in the region of 1 KHz by choice of an appropriate AC magnetic bias field, so as to reduce the sensor's susceptability to vibration.

The ability to construct the sensor with adequate sensitivity using a short length of optical fibre enables its mechanical resonant frequency to be substantially raised.

If an addition the mechanical resonant fre- quency and the frequency of the applied magnetic field are similar the sensitivity of the sensor is found to be enhanced. As fibres are normally protected by a thin mechanically lossy coating which reduces the mechanical coupling between the fibre and the arcuate element and thus the maximum possible sensitivity, this has particular advantage.

It will be appreciated that whilst in the sensor and interferometer described hereinbefore by way of example the sensor is arranged to monitor changes in a DC magnetic field in the presence of an AC bias field so as to achieve optimum sensitivity generally a sensor in accordance with the invention will be responsive to any change in applied magnetic field.

It will also be appreciated that in some applications a gradiometer employing two parallel triads of three orthogonal sensors in accordance with the invention may be useful. Each pair of sensors within a pair of parallel planes would be separated by a known displacement, the magnetic field gradient in a direction normal to the planes being obtained from the difference in outputs obtained from each of the pair.

Claims

1. A magnetic field sensor comprising an arcuate element comprising two superimposed elongate strips of material, the magnetostrictive constant along the longitudinal axis of one of the strips being greater than that of the other strip; and means for attaching an optical fibre along a chord of the element such that a variation in applied magnetic field in the plane containing the arc of the element gives rise to a variation in the curvature of the element so as to produce a variation in the strain in the fibre.

2. A sensor according to Claim 1 in which the means for attaching comprises a pair of posts, one at each end of the chord.

3. A sensor according to Claim 2 in which the posts project from said other strip.

4. A sensor according to any one of the preceding claims in which the material of said one strip is a metallic glass.

5. A sensor according to any one of the preceding claims in which the fibre forms part of a Mach-Zehnder interferometer arranged to monitor changes in optical phase of light passing through the fibre.

6. A magnetic field sensor substantially as hereinbefore described with reference to the accompanying draWings.

Printed in the United Kingdom for Her Majesty's Stationery Office, Dd 8818935, 1986, 4235. Published at The Patent Office, 25 Southampton Buildings, London, WC2A lAY, from which copies may be obtained.